To determine the value of \(x\) for the torsional constant of the suspension wire, we begin by considering the dynamics of a moving coil galvanometer. The torque \(\tau\) on the coil due to current \(I\) is given by:
\[\tau = n \cdot B \cdot A \cdot I\]
where \(n\) is the number of turns, \(B\) is the magnetic field, \(A\) is the area of each turn, and \(I\) is the current.
Substituting the given values: \(n = 100\), \(B = 0.01 \, \text{T}\), \(A = 2.0 \times 10^{-4} \, \text{m}^2\) (converted from cm² to m²), and \(I = 10 \times 10^{-3} \, \text{A}\), we calculate:
\[\tau = 100 \times 0.01 \times 2.0 \times 10^{-4} \times 10 \times 10^{-3} = 2 \times 10^{-5} \, \text{N} \cdot \text{m}\]
The torsional constant \(k\) relates the torque to the angular deflection \(\theta\) as \(\tau = k \cdot \theta\). Given \(\theta = 0.05\) radians, we substitute to find \(k\):
\[2 \times 10^{-5} = k \times 0.05\]
Solving for \(k\):
\[k = \frac{2 \times 10^{-5}}{0.05} = 4 \times 10^{-4} \, \text{N} \cdot \text{m/rad}\]
The torsional constant is expressed as \(x \times 10^{-5}\), so equating \(4 \times 10^{-4} \) to \(x \times 10^{-5}\) gives:
\[x \times 10^{-5} = 4 \times 10^{-4}\]
\(x = 4\)
Given: - Number of turns: \(N = 100\) - Area of each turn: \(A = 2.0 \, \text{cm}^2 = 2.0 \times 10^{-4} \, \text{m}^2\) - Magnetic field: \(B = 0.01 \, \text{T}\) - Deflection: \(\theta = 0.05 \, \text{radian}\) - Current: \(I = 10 \, \text{mA} = 10 \times 10^{-3} \, \text{A}\)
The torque (\(\tau\)) acting on a moving coil galvanometer is given by:
\[ \tau = N \times B \times I \times A \]
Substituting the given values:
\[ \tau = 100 \times 0.01 \, \text{T} \times 10 \times 10^{-3} \, \text{A} \times 2.0 \times 10^{-4} \, \text{m}^2 \] \[ \tau = 100 \times 0.01 \times 0.01 \times 2.0 \times 10^{-4} \, \text{N} \times \text{m} \] \[ \tau = 2 \times 10^{-5} \, \text{N} \times \text{m} \]
The torque is also related to the torsional constant (\(k\)) and deflection (\(\theta\)) by:
\[ \tau = k \times \theta \]
Rearranging to find \(k\):
\[ k = \frac{\tau}{\theta} \]
Substituting the given values:
\[ k = \frac{2 \times 10^{-5}}{0.05} \, \text{N} \times \text{m/rad} \] \[ k = 4 \times 10^{-4} \, \text{N} \times \text{m/rad} \]
Given that \(k = x \times 10^{-5} \, \text{N} \times \text{m/rad}\):
\[ 4 \times 10^{-4} = x \times 10^{-5} \]
Solving for \(x\):
\[ x = 4 \]
Conclusion: The value of \(x\) is 4.
| Group-I | Group-II | ||
| P | Magnetic | 1 | Chargeability |
| Q | Gravity | 2 | Electrical conductivity |
| R | Magnetotelluric | 3 | Susceptibility |
| S | Induced Polarization | 4 | Density |
Consider the sound wave travelling in ideal gases of $\mathrm{He}, \mathrm{CH}_{4}$, and $\mathrm{CO}_{2}$. All the gases have the same ratio $\frac{\mathrm{P}}{\rho}$, where P is the pressure and $\rho$ is the density. The ratio of the speed of sound through the gases $\mathrm{v}_{\mathrm{He}}: \mathrm{v}_{\mathrm{CH}_{4}}: \mathrm{v}_{\mathrm{CO}_{2}}$ is given by